US5851062A - Prism sheet for surface light source - Google Patents

Abstract

A periodic pattern is formed on a surface of prism sheet, and the cross section of a minimal unit 14 of the periodic pattern is shaped like an M. The M-shape includes a long positive-sloping surface, a short negative-sloping surface, a short positive-sloping surface and a long negative-sloping surface 16b. By designing the prism sheet in such a manner, a portion of the light behaving in a side mode is converted to recurrent mode light, and the surface luminance is enhanced.

Description

FIELD OF THE INVENTION

This invention relates to a prism sheet for a surface light source which increases the luminance by reducing the amount of light beams that are emitted outside of a desired field of view. The surface of the prism sheet is designed so as to condense the incoming light efficiently. This kind of surface light source can be used for surface-type optical elements (for example, an LCD) which are widely employed for use as an image display, a display screen for a computer display, a data terminal, a TV receiver, a video camera and a head-mounting display.

BACKGROUND OF THE INVENTION

Liquid crystal display (LCD) panels have the characteristics of being thin and light-weight. Because of these qualities, they have come to be widely used in recent years for such applications as notebook or book-type personal computers, display screens for portable TVs, displays for portable terminal devices and terminal equipment for display purposes.

However, as liquid crystal display panels are not themselves capable of emitting light, a separate surface light source must be provided for the display. Since most portable devices such as notebook-type personal computers or appliances like portable TVs are battery-driven, there is a demand for a long battery life. This leads to a preference for efficient use of photoemissive power.

FIG. 1 is an exploded perspective view of a conventional surface light source A, which is used with a liquid crystal display panel. Surface light source A has adiffusion panel 2 and aprism sheet 3 above aphotoconductive panel 1, and areflective sheet 4 below thepanel 1. On the side ofpanel 1 is alinear light source 5, which is shown as a fluorescent lamp.Prism sheet 3 has a periodic pattern which is repeated uniformly in one direction and runs perpendicular to that direction. The minimal unit of this periodic pattern is atriangular prism 6 with two surfaces. Generally, the cross section of theprism 6 is an isosceles triangle with base angles of 45° or 40°, and these triangles are arrayed in a single dimension. To produce a uniform intensity of reflected light, a pattern is formed on the surface ofreflective sheet 4 which includes portions which reflect directly and other portions which reflect diffusely, both arranged at an appropriate density pattern.

The light produced bylinear light source 5 is conducted from the lateral surface ofphotoconductive panel 1 to its interior and reflected upward byreflective sheet 4. The light emitted from the upper surface ofconductive panel 1 is diffused at a uniform brightness bydiffusion panel 2.Prisms 6 ofprism sheet 3 condense the light diffused bypanel 2 to increase its luminance.

Theprism sheet 3 provided in surface light source A as described above reduces horizontal leakage by condensing the light and thereby enhances the efficiency with which the light is used. To ascertain the effect ofprism sheet 3, the angular dependency (the directional characteristic) of the luminance with and withoutprism sheet 3 was measured. The result is shown in FIG. 2. If the horizontal axis Θ_x represents direction Z, the direction of radiation with respect to the upper surface ofprism sheet 3, and the X axis represents the direction in which the periodic pattern is arrayed, then the angle measured is the one formed by the Z axis at surface Z-X (the angle is positive in the positive direction of the X axis) (See FIG. 1). The vertical axis represents relative luminance. Broken line b represents the angular dependency of the relative luminance (of the light conducted by conductive panel 1) whenprism sheet 3 is not used, and solid line a represents the angular dependency of the relative luminance (of the light which exits prism sheet 3) whenprism sheet 3 is used.

As is made clear by FIG. 2,prism sheet 3 condenses the light which exitsconductive panel 1 into a comparatively narrow range (in the example shown in FIG. 2, from -45° to +45°). Since most of the systems which use a liquid crystal display are for personal use, the angles of view which are most frequently employed will fall in the range of ±30° to ±45°. Installing aprism sheet 3 in surface light source A causes the light outside the field of view to be channeled into it, thereby increasing the luminance on the front of the liquid crystal display panel. This is precisely whyprism sheets 3 are used in surface light sources A.

However, when the solid line a in FIG. 2 is looked at in detail, it is apparent that it has a secondary peak p on either end (at approximately ±75°). Even when aprism sheet 3 is used in surface light source A, then, a great deal of the light travels outside of the targeted angle of view. The light emitted beyond this angle of view is wasted.

If the behavior of alight beam 7 which strikes an existingprism sheet 3 is analyzed, one finds that it can be divided into three modes of behavior of light rays according to the angle of incidence. These are shown in FIGS. 3 (a), 3 (b), 3 (c), 3 (d) and 3 (e). FIG. 3 (a) shows the luminance (i.e., the directional characteristic) for each optical path of the light which passes throughdiffusion panel 2, as expressed by Lambert's law. The beams which pass throughdiffusion panel 2 andstrike prism sheet 3 exhibit three modes of behavior: a front mode, a recurrent mode and a side mode.

In the front mode, which is shown in FIG. 3 (c), beams which enterprisms 6 from below strike the oblique surfaces of those prisms at an angle of incidence which is smaller than the angle of total internal reflection. They are refracted and emitted to the exterior via the oblique surfaces ofprisms 6. The front mode is the mode for whichprism sheet 3 is designed. The majority of thebeams 7 which pass throughprism sheet 3 exhibit front mode behavior. In this mode, as can be seen in FIG. 3 (c), the spreading of the beams transmitted byprisms 6 is checked, and a directional characteristic can be achieved such that the luminance is high at the front (see FIG. 3 (e)).

In the recurrent mode, as shown in FIG. 3 (d), thebeams 7 which enterprisms 6 are reflected twice by the oblique surfaces of those prisms, re-emitted via the lower surface ofprisms 6 and returned toconductive panel 1. Thebeams 7 which return are reflected bypanel 1 at luminance k (due to scattering and other losses, k=0.9, typically) and returned once again toprism sheet 3. Most of these recycledbeams 7 are converted to front mode beams which strikeprisms 6.

In the side mode, as shown in FIG. 3 (b), thebeams 7 which enterprisms 6 are reflected by one of the oblique surfaces of the prism and refracted by the opposite oblique surface as they are transmitted to the exterior. Since the path of thebeams 7 emitted in the side mode is approximately 90° off the normal path (i.e., Θ_x =approximately ±90°), they are effectively useless. The two peaks p in solid line a shown in FIG. 2 represent the beams travelling in side mode.

Of the three modes of behavior, then, the side mode is the most crucial in improving the function of the prism sheet. If the number of beams which exhibit side mode behavior can be reduced, then the number of beams which exit the prism at a large angle can be minimized, thereby increasing the frontal luminance.

SUMMARY OF THE INVENTION

This invention is developed in consideration of the technical background discussed above. Its objective is to reduce the number of beams which exit a prism sheet covering a surface light source in a side mode so as to improve the frontal luminance.

The prism sheet of a surface light source described in this invention is distinguished by the following. It comprises a surface which has a periodic pattern consisting of regularly repeated angled edges like M-shaped pattern. A cross section of one of the minimal units of the periodic pattern characterizing this prism sheet has at least four surface slopes, each of which has a slope which is opposite the next.

In this prism sheet, the minimal unit of the periodic pattern has at least four surface slopes which are arranged in such a way that each surface slops faces opposite the next. That is, surface slopes with positive and negative slopes vis-a-vis the surface direction of the prism sheet are arranged to each other. The central two surface slopes out of four are shorter than the other two, and these two shorter slopes constitute a shallow groove in each periodic pattern. Thus, a portion of the beam which is reflected by one surface and transmitted by another surface will reenter the prism sheet via the third surface and be reflected by the fourth surface opposite the third surface. In this way, the beam will be made to assume a recurrent mode.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a perspective drawing of a surface light source covered with a conventional prism sheet.

FIG. 2 is a graph of the angular distribution (the directional characteristic) of the luminance of the same surface light source.

FIGS. 3 (a), 3 (b), 3(c), 3 (d), and 3 (e) illustrate the three modes of behavior (side mode, FIG. 3 (b); front mode, FIG. 3 (c); recurrent mode, FIG. 3 (d)) of light beams.

FIG. 4 is a perspective drawing of a surface light source covered with a prism sheet designed according to this invention.

FIG. 5 illustrates the effect of the prism sheet in the same surface light source.

FIG. 6 (a) illustrates how front mode light behaves with respect to a prism sheet according to this invention.

FIG. 6 (b) illustrates how front mode light behaves with respect to a conventional prism sheet.

FIG. 7 (a) illustrates how recurrent mode light behaves with respect to a prism sheet according to this invention.

FIG. 7 (b) illustrates how recurrent mode light behaves with respect to a conventional art prism sheet.

FIG. 8 (a) illustrates how side mode light behaves with respect to a prism sheet according to this invention.

FIG. 8 (b) illustrates how side mode light behaves with respect to a conventional prism sheet.

FIG. 9 shows a portion (the minimal unit) of a prism sheet which is another ideal embodiment of this invention.

FIG. 10 illustrates the relationship between the dimensions of above prism sheet.

FIG. 11 shows a portion (the minimal unit) of a prism sheet which is another ideal embodiment of this invention.

FIGS. 12 (a) and (b) illustrate the effect of a portion (the minimal unit) of a prism sheet which is another ideal embodiment of this invention.

FIG. 13 illustrates the behavior of light in secondary side mode.

FIG. 14 (a) illustrates the configuration which converts a portion of the light in secondary side mode as described above to recurrent mode.

FIG. 14 (b) is provided for comparison to FIG. 14 (a).

FIG. 15 (a) is a perspective drawing of a surface light source covered with a prism sheet which is another ideal embodiment of this invention.

FIG. 15 (b) is an enlarged cross section taken along line k--k in (a).

FIG. 16 (a) is a perspective drawing of a surface light source covered with a prism sheet which is another ideal embodiment of this invention.

FIG. 16 (b) is an enlarged cross section taken along line n₁ --n₁ in (a). (c) is an enlarged cross section taken along line n₂ --n₂ in (a).

FIG. 17 is a perspective drawing of a surface light source covered with two prism sheets which is another ideal embodiment of this invention.

FIG. 18 (a) is a perspective drawing of a surface light source covered with a prism sheet which is another ideal embodiment of this invention.

FIGS. 18 (b) through (d) illustrate the shape of the continuous pattern in different locations on the prism sheet.

FIG. 19 is a block diagram of an image display incorporated with a prism sheet.

DETAILED DESCRIPTION OF THE INVENTION

FIG. 4 shows a surface light source B covered with a prism sheet, according to a first embodiment of this invention. Surface light source B includes backlight unit (light source) 11 and surface-type prism sheet 112. A diffusion panel may be placed betweenbacklight unit 11 andprism sheet 112, or a diffusion panel or sheet may be provided on the surface of the light source to diffuse the light. Another alternative would be to diffuse the light with a diffusion panel or sheet on the undersurface ofprism sheet 112.Backlight unit 11 emits light toward its upper surface, on whichprism sheet 112 is placed.

The upper surface ofprism sheet 112 includes deep V-shapedgrooves 13a and shallow V-shapedgrooves 13b, which alternate with respect to each other. The M-shaped portion between each pair ofdeep grooves 13a is an M-shapedprism 14, the minimal unit of the periodic pattern. The periodic pattern ofprism sheet 112, then, extends uniformly along the Y axis and includes a repeated series of the M-shapedprisms 14 which are its minimal units along the X axis.Minimal units 14 include along surface slope 15a, which has a positive slope (for the purpose of explanation, inclinations which go up toward the right in the drawing are referred to as positive, and those which go down toward the right are referred to as negative); ashort surface slope 16a, which has a negative slope; ashort surface slope 15b, which has a positive slope; and along surface slope 16b, which has a negative slope (See FIG. 5). It is not necessary that 15a and 15b, the surface slopes with positive slopes, and 16a and 16b, the surface slopes with negative slopes, have exactly the same slope. If they do, however, it will be easier to design the shape of the periodic pattern forprism sheet 112.

With this sort of pattern of repeated M-shapes, the light beams 7 which strike the prism sheet in the side mode and so are wasted in conventional light sources are converted to recurrent mode beams. The recurrent mode light is re-reflected and becomes front mode light, so the frontal luminance of surface light source B is increased. FIG. 5 illustrates the effect of aprism sheet 112 designed according to the invention.Basic unit 14 ofprism sheet 112 and the path along which it conductslight beam 7 are drawn in solid lines.Prism 6 ofconventional prism sheet 3 of FIG. 1 and the path along which it conductslight beam 7 are drawn in broken lines. Withconventional prism 6, the beam of light reflected bysurface 15a will strike the opposite surface, 16b, at an angle of incidence which is smaller than the angle of total internal reflection. As a result, it will be conducted to the exterior bysurface 16b as side mode light. Thebasic unit 14 of the periodic pattern of the invention, however, has a shallow V-shapedgroove 13b in its center. The light beam reflected bylong surface 15a will exit from the nextshort surface 16a and enterminimal unit 14 via the oppositeshort surface 15b. When it passes through the two short surfaces, 16a and 15b, the light beam is refracted. The angle of incidence at the opposite long surface, 16b, thereby becomes larger than the angle of total internal reflection, so thatlight beam 7 is reflected downward bylong surface 16b and assumes the recurrent mode. Aprism sheet 112 with a periodic pattern as per the invention, then, will have increased frontal luminance, and the efficiency with which the light is used will be enhanced.

A comparison is made between the effects of theconventional prism sheet 3 and theprism sheet 112 according to the invention, with respect to each mode of light. To simplify the explanation, in FIGS. 6 through 8, the surfaces with positive slopes, 15a and 15b, have been made parallel with respect to each other, and the surfaces with negative slopes, 16a and 16b, have been made parallel with respect to each other.

The behavior of light in the front mode which passes through positive-slopingsurface 15a in theconventional prism sheet 3 is shown in FIG. 6 (b). The behavior of light in the front mode with respect toprism sheet 112 of the invention is shown in FIG. 6 (a). In the periodic pattern of the invention shown in FIG. 6 (a), alllight beams 7 assume the front mode. In both FIGS. 6 (a) and 6 (b), the light in the front mode is transmitted along the same diffraction path, and the total quantity of light in front mode is identical. The circled numbers indicate the corresponding regions of the light beams.

FIG. 7 (b) shows the behavior of light in the recurrent mode which is reflected by positive-slopingsurface 15a in theconventional prism sheet 3. FIG. 7 (a) shows the behavior of the correspondinglight beams 7 with respect toprism sheet 112 of the invention. With the periodic pattern of the invention shown in FIG. 7 (a), the light which strikes region (1) is returned to region (1); that which strikes region (2) is returned to region (2); and that which strikes region (3) is returned to region (3). Just as in the example from the conventional case, all the light assumes the recurrent mode. The quantity of light which recurs is the same in FIGS. 6 (a) and 6 (b), so the total quantity of light in the recurrent mode is the same.

FIG. 8 (b) shows the behavior of light in the side mode which is reflected by positive-slopingsurface 15a in theconventional prism sheet 3. FIG. 8 (a) shows the behavior of the correspondinglight beams 7 with respect toprism sheet 112 of the invention. In the example of the conventional case shown in FIG. 8 (b), thebeams 7 in regions (1), (2) and (3) all assume the side mode. With the prism sheet shown in FIG. 8 (a), the light in region (2) is reflected bylong surface 15a and exits in the side mode from the opposite short surface, 16a. The light in region (3) is reflected byshort surface 15b and exits in the side mode from the opposite long surface, 16b. The light in region (1), however, is reflected by positive-slopinglong surface 15a, passes throughshort surfaces 16a and 15b, is reflected bylong surface 16b and conducted downward in the recurrent mode.

When theprism sheet 112 of the invention is employed, then, the light beams which assumed the front or recurrent mode when they encountered theconventional prism sheet 3 assume those same modes, and a portion of the light beams which would be wasted in the side mode by a conventional prism are converted into the recurrent mode light. Theprism sheet 112 of the invention reduces the quantity of light lost in the side mode and increases the quantity of light which assumes the recurrent mode. The result is that the quantity of light which assumes the front mode is increased.

When shallow V-shapedgroove 13b is designed using theconventional prism sheet 3 as a starting point, a designer need not consider the light in the recurrent or front mode. Since his or her only problem is how to reduce the quantity of light in the side mode, the design process is simplified.

FIG. 9 shows a portion (minimal unit 21) of the periodic pattern ofprism sheet 122 of a second embodiment of this invention. The minimal unit of this periodic pattern has a deep V-shapedgroove 13a on either end which separates it from the next minimal unit. Between these twodeep grooves 13a is anintermediate groove 13b, which is separated from the deep grooves by twoshallow grooves 13c. Thus, eachminimal unit 21 has eight surfaces with positive and negative slopes arranged alternately.

This configuration is equivalent to providing two additionalshallow grooves 13c on the apices on either side ofshallow groove 13b in theminimal unit 14 shown in FIG. 5 (intermediate groove 13b in FIG. 10). With this configuration, as can be seen in FIG. 10, the proportion of the side mode light which is converted to the recurrent mode can be increased.

If additional shallow grooves are created on the four apices of aminimal unit 21 produced in the way shown in FIG. 10, the proportion of the side mode light converted to the recurrent mode can be further increased. By repeating this process, one could continue endlessly to increase the number of grooves. However, increasing the number of grooves would result in an extremely detailed periodic pattern, which would make it difficult to manufacture prism sheet.

When the width of aminimal unit 21 in the periodic pattern approaches the period of a pixel in the liquid crystal display panel, a moire will result. For this reason, the width W₁ normally chosen for a minimum unit is 30 μm, as shown in FIG. 10. Ifminimal unit 21 has only asingle groove 13b, the width W₂ of one surface of that groove will be 5 μm. Ifunit 21 has three grooves, 13c, 13b and 13c, the width W₃ of one surface of ashallow groove 13c will be 1 μm. When a form is produced forprism sheet 122 in a cutting process, the edge portions of the pattern in the form take on a sub-micron roundness, which offsets the effect of increasing the number of grooves. When one compares the effective use of the light with the ease of producing the form, it seems most desirable to make aprism 112 whoseminimal unit 14 has four surfaces and only one V-shaped groove, as shown in FIG. 6 (a).

FIG. 11 shows theminimal unit 22 in the periodic pattern ofprism 132 according to a third embodiment of the invention. Theminimal unit 22 of this periodic pattern has six positive- and negative-sloping surfaces, 15a, 15b, 15c, 16a, 16b and 16c, arranged alternately. The two central surfaces, 15b and 16b, are longer than the surfaces on their distal sides, 16a and 15c. The unit is symmetrical left to right. Thisminimal unit 22 can be achieved by forming a V-shapedgroove 13b on either side of the apex in the center of aconventional prism 6, which has a triangular cross section. In the third embodiment, too, the design process can be simplified if the positive-sloping surfaces, 15a, 15b and 15c, are all made parallel to with respect each other, and the negative-sloping surfaces, 16a, 16b and 16c, are also made parallel with respect to each other.

In thisprism 132, theminimal unit 22 is symmetrical left to right, so it can reduce the light in the side mode from the left and right sides equally. It has only two V-shapedgrooves 13b, so its smallest surfaces, 16a and 15c, are not so short that it is impossible to produce a basic form for the prism sheet.

FIGS. 12 (a) and (b) show theminimal unit 23 in the period pattern of anotherprism 142 according to a fourth embodiment of the invention. Theminimal unit 23 of this periodic pattern has four positive- and negative-sloping surfaces, 15a, 15b, 16a and 16b, arranged alternately. The distal surfaces, 15a and 16b, are of different lengths, as are the proximal surfaces, 15b and 16a. Thisminimal unit 23 can be achieved by forming on the apex of a conventional triangular prism 6 a V-shapedgroove 15b which is biased to either the left or right.

As is shown in FIG. 12 (a), aprism 142 whoseminimal unit 23 has a biased V-shapedgroove 23 in its center will convert to the recurrent mode a high proportion of the side mode light which strikes the shorter side ofgroove 13b. As is shown in FIG. 12 (b), it will convert to the recurrent mode a much smaller proportion of the side mode light which strikes the longer side of the groove.

It is desirable, then, to shiftgroove 13b off center as in the third embodiment when there is significantly more side mode light striking one side of the prism. FIG. 15 (a) shows surface light source C₁, which has abacklight unit 11 with alight source 25 on one side to provide light radiating from the edge. When this sort ofbacklight 11 is used, the luminance is greatest in direction L, the direction faced by the side of the prism oppositelight source 25. For this reason, the periodic pattern ofprism 142 should have aminimal unit 23 oriented as shown in FIG. 15 (b). (This figure shows the shape ofminimal unit 23 in a cross section taken along line k--k in FIG. 15 (a).)

FIG. 13 illustrates the behavior of secondary side mode light. Depending on the shape and refractive index of theconventional prism 3, it will produce secondary side mode light which behaves differently from that shown in FIG. 3 (b). Secondary side mode is pictured in FIG. 13. Alight beam 7 which entersprism 6 is reflected by one oblique surface of that prism and refracted by the opposite oblique surface. The beam exits to the exterior as primary side mode light but then strikes thenext prism 6. It is totally reflected by the undersurface ofprism 3 and exits the side ofprism 6 virtually parallel toprism 3.

FIG. 14 (b) shows the behavior of this secondary side mode light with respect to aminimal unit 23 which is symmetrical left to right and has ashallow groove 13b in its center. All thelight beams 7 which strikeprism 112 in regions (1) through (3) are totally reflected by its undersurface and exit as secondary side mode light. Aminimal unit 23 with this configuration, then, is incapable of converting secondary side mode light to the recurrent mode.

One can address this secondary side mode light by making aminimal unit 23 with ashallow groove 13b biased to either the left or right on the apex of a conventionaltriangular prism 6, just as in FIG. 12 (a). This will allow one to convert a portion of the secondary side mode light to the recurrent mode. As can be seen in FIG. 14 (a), the light beams 7 which strike the undersurface ofprism 142 in regions (1) and (3) are totally reflected by the undersurface and assume the side mode, just as in FIG. 14 (b). Thebeams 7 which strike region (2), however, reenterprism 142 and exit to the exterior via the undersurface as recurrent mode light.

It is therefore desirable to offsetgroove 13b from the center ofminimal unit 23, as in FIG. 14 (a), when there is a considerable quantity of secondary side mode light. Theshallow groove 13b is oriented in opposite ways in FIGS. 12 (a) and 14 (a). In FIG. 12 (a),groove 13b is shifted so that it faces opposite the direction in which the side mode light is travelling when it exits the prism. In FIG. 14 (a), the groove is shifted to face the direction in which the secondary side mode light will exit the prism. In situations where there is both primary side mode light which does not strike the prism again and secondary side mode light which does, the user must ascertain which type of side mode light is more prevalent in order to determine in whichdirection groove 13b should be shifted. If one considers the secondary side mode light with respect to surface light source C₁ shown in FIG. 15 (a), there will be cases in whichgroove 13b should be shifted opposite to the way shown in FIG. 15 (b).

The angles α and β whichdistal surfaces 15a and 16b make with respect to the lower surface of the prism (see FIG. 14 (b)) are related to the distribution of the luminance produced by the light source. These angles need not be identical (i.e., do not need to require α=β), and appropriate values may be selected for them.

FIG. 16 (a) is a perspective drawing of surface light source C₂, according to a fifth embodiment of this invention. Light source C₂ has twobacklight units 11, each with alight source 25, to provide edge lighting on two sides.Prism 142 has a periodic pattern consisting of asymmetricalminimal units 23 as shown in FIG. 12. The periodic pattern is uniform in the plane diagonal toconductive panel 24. Consider two cross sections which are both perpendicular tolight sources 25 inprism 142. The cross section in FIG. 16 (b) (taken along line n₁ --n₁ in FIG. 16 (a)) and that in FIG. 16 (c) (taken along line n₂ --n₂ in the same figure) are each asymmetrical with respect to one oflight sources 25. In this case, just as in FIG. 15, whichway groove 13b should be biased will depend on the user's decision whether to address primary or secondary side mode light.

FIG. 17 is a perspective drawing of surface light source C₃, according to a sixth embodiment of the invention. Light source C₃ has twobacklight units 11, each with alight source 25, to provide edge lighting on two sides, and twoprism 112. Oneprism 112 has a periodic pattern which is uniform in parallel to one of the light sources. The other has a pattern which is uniform in parallel to the other light source. The minimal unit of the periodic pattern may be of any shape, so the user may selectminimal unit 14 in FIG. 4,unit 21 in FIG. 10,unit 22 in FIG. 11 orunit 23 in FIG. 12.

When the angular distribution of the luminance of the light radiated by the conductive panel varies with the location, the characteristics of the minimal unit shown in FIG. 12 may be employed so that the cross section of the continuous pattern will vary with its location. FIG. 18 (a) shows surface light source C₄, which has abacklighting unit 11 with twolight sources 25 on opposite sides ofconductive panel 24 to provide edge lighting. Inbacklighting unit 11, as can be seen in the drawing, theluminance 26 in the vicinity oflight sources 25 is greater on the paths which angle back toward the light sources than on the paths which angle away from them, and the angular distribution of theluminance 26 in the center ofconductive panel 24 is symmetrical. In such a case, the V-shapedgrooves 13b on the ends ofprism 112 which are close tolight sources 25 should be biased so thatsurface 27 faces away from the nearer light source. In the middle ofprism 112grooves 13b should be directly centered between twoequal surfaces 27. As an alternative, the shape of the minimal units inprism 112 could be varied gradually from the extremities toward the center. FIGS. 18 (b), (c) and (d) show three such minimal units forprism 112. FIGS. 18 (b) and (d) are units which would be used inlocations 28a and 28c; FIG. 18 (c) would be used inlocation 28b in FIG. 18 (a).

Surface light source B discussed above can be employed in a variety of image displays. FIG. 19 is a block diagram of image display D, a device which employs a surface light source B designed according to the invention. In response to an input signal,panel 81 converts the virtually uniform light emitted by surface light source B into a black and white or color image which it displays.Panel 81 may, for example, be a liquid crystal display panel.Input interface 82 converts the input signal to a signal whichpanel 81 can process.Power supply 83 supplies electrical power todriver 84 to drive surface light source B,input interface 82 andpanel 81.

These image displays employing the surface light source are widely used in various types of image display devices, projection devices, head-mounting displays, non-portable and portable liquid crystal televisions (TV receivers), video cameras, and data terminals. Using a prism sheet designed according to this invention in any of these devices will result in higher surface luminance and improved legibility.

With the prism sheet according to the invention, a portion of the light which is emitted horizontally in the side mode and so wasted by a conventional art prism is converted to light of recurrent mode. Most of this recurrent mode light is then converted to front mode light. With the surface light source having the prism of the invention, then, the quantity of useless side-mode light is reduced and the quantity of front-mode light is increased. This allows us to achieve a surface light source with a high frontal luminance.

Claims (10)

What is claimed is:

1. A surface-type prism sheet having a shape of a periodic pattern for use with a surface light source, each periodic pattern comprising:

a plurality of surfaces extending to one direction,

wherein a cross section of said each periodic pattern has at least four surface slopes extending to an orthogonal direction with respect to adjacent surface slopes of said each periodic pattern, each of said at least four surface slopes faces opposite to said adjacent surface slopes of said each periodic pattern,

wherein said at least four surface slopes of said each periodic pattern include two distal surfaces having first cross sectional widths and two proximal surfaces having second cross sectional widths different from said first cross sectional widths, and

wherein said first cross sectional width is longer than said second cross sectional width.

2. A surface-type prism sheet according to claim 1, wherein said cross section of said each periodic pattern is configured by a plurality of positive and negative sloping surfaces in an alternating arrangement, said positive sloping surfaces being parallel to each other, and said negative sloping surfaces being parallel to each other.

3. A surface-type prism sheet according to claim 1, wherein said each periodic pattern of said prism sheet has six surfaces, two central surfaces of said six surfaces being of longer cross sectional widths than two intermediate surfaces of said six surfaces, said two intermediate surfaces being situated on distal sides of said two central surfaces, respectively,

wherein two V-shaped grooves are formed in said each periodic pattern between respective ones of said intermediate surfaces and said central surfaces of said each periodic pattern.

4. A surface-type prism sheet according to claim 3, wherein each of said two V-shaped grooves in said each periodic pattern has a depth less than a depth at end portions of said each periodic pattern.

5. A surface-type prism sheet according to claim 1, wherein said surface slopes differ from place to place in such a way to counteract a variation of an incoming light emission in order to make uniform an intensity of outgoing light from said prism sheet.

6. A surface-type prism sheet according to claim 1, wherein said each periodic pattern of said prism sheet has eight surfaces, two central surfaces of said six surfaces being of longer cross sectional widths than two respectively adjacent first intermediate surfaces of said six surfaces, said each periodic pattern including second intermediate surfaces of said six surfaces respectively adjacent to said first intermediate surfaces of said six surfaces,

said each of said periodic patterns including two distal surfaces respectively adjacent to said second intermediate surfaces of said six surfaces,

wherein three V-shaped grooves are formed in said each periodic pattern, each of said three V-shaped grooves having a respective depth less than a depth of said each periodic pattern at respective beginning and ending points of said each periodic pattern.

7. A surface-type prism sheet according to claim 1, wherein a V-shaped groove is created in said each periodic pattern by said two proximal surfaces, said V-shaped groove having a groove depth less than a depth of said each periodic pattern defined at starting and ending points of said each periodic pattern that are respectively located at end points said distal surfaces of said each periodic pattern that are furthest away from said proximal surfaces of said each periodic pattern.

8. A surface-type prism sheet according to claim 1, wherein said at least four surface slopes extend along a substantially perpendicular direction with respect to said adjacent surface slopes of said each periodic pattern.

9. A surface-type prism sheet according to claim 1, wherein said first cross sectional widths of said two distal surfaces include a first and second cross sectional width different from each other, and

wherein said second cross sectional widths of said two proximal surfaces include a first and second cross sectional width different from each other.

10. A surface-type prism sheet having a shape of a periodic pattern of prisms for use with a surface light source, said prism sheet having a substantially planar bottom surface and a top surface on which said periodic pattern of prisms are disposed, each of said prisms comprising:

a first point and a second point defining beginning and ending points of said each prism; and

a V-shaped groove disposed in said each prism between said first point and said second point,

wherein said V-shaped groove has a depth such that said first and second points are closer to said substantially planar surface of said prism sheet than any portion of said V-shaped groove.

Images